Yiyi Ji1, Werner Hoffmann2, Michal Pham1, Celal Oezerdem1, Helmar Waiczies3, Thoralf Niendorf1,3,4, and Lukas Winter1
1Berlin Ultrahigh Field Facility (B.U.F.F.), Max Delbrück Center for Molecular Medicine in the Helmholtz Association (MDC), Berlin, Germany, 2Physikalisch-Technische Bundesanstalt (PTB), Berlin, Germany, 3MRI.TOOLS GmbH, Berlin, Germany, 4Experimental and Clinical Research Center (ECRC), a joint cooperation between the Charité Medical Faculty and the Max Delbrück Center for Molecular Medicine in the Helmholtz association
Synopsis
An integrated RF heating
system utilizes the MR spin excitation frequency together with dedicated RF
antennas for controlled RF heating and MR imaging in an integrated system.
Operating the MR power amplifier for both RF heating and MR imaging
applications simultaneously requires customized transmit/receive (Tx/Rx)
switches that can handle both high peak powers and high average powers. In this
work we designed, built and evaluated a high power Tx/Rx switch for handle MRI
and RF heating requirements.
Introduction
Controlled
application of thermal dose is of major interest in thermal phenotyping, multimodal
RF hyperthermia treatments, thermal drug release and MR safety evaluations [1-3].
An integrated RF heating system utilizes the spin excitation frequency for
controlled RF induced heating and MR imaging [4-5]. Operating the MR power
amplifier for RF heating and MRI simultaneously requires customized transmit/receive
(Tx/Rx) switches, which can protect the preamplifiers from high peak powers and
withstand high average power of >50-100W. Traditional Tx/Rx switches commonly
use pin diodes to switch between transmit and receive modes, which constraints
the average power to <25W. To address this shortcoming we designed, built
and evaluated a high power Tx/Rx switch tailored to be driven at much larger
average power.Materials and Methods
The schematic of the proposed high power Tx/Rx
switch is presented in Fig.1a. It
consists of three λ/4 stubs assembled with semi-rigid coaxial cables for 297MHz
and two pin diodes (D1: Tx path, D2: Rx path, MA4P7441F-1091T, Macom, MA, USA). A LC resonant circuit tuned
to 297MHz is placed between each pin diode and λ/4 stub to afford maximum
isolation between the Tx and Rx paths. The Tx and Rx path circuits were placed
in double shielded compartments to increase isolation (Fig.1b). During Tx mode, a short in point 1 and 4 (Fig.1a) is transformed into an open in
point 2 and 3 by λ/4 stubs so that all RF signal is routed into the RF coil.
During Rx mode, an open in point 4 translates into a short in point 3 and an
open in point 2, directing the signal into the Rx port.
Temperature in the Tx/Rx switch circuit while
driving Pavg=85W was accessed with an infrared camera (Ti25,
Fluke, WA, USA).
An experimental setup comprising a rectangular phantom
(90×180×260mm3) with cylindrical sample holders and a bow tie dipole
antenna for transmission [4] (Fig.2a-b)
was used to examine the suitability of the high power Tx/Rx switch for MR
imaging and RF heating in a B0=7.0T MR system (Magnetom, Siemens Healthcare,
Erlangen, Germany). MR images were acquired using a gradient echo sequence (FOV=(240×240)mm2,
TR=8.6ms, TE=4.7ms, spatial resolution=(1.0×1.0×5.0)mm3) with i)
the proposed high power Tx/Rx switch and ii) a conventional Tx/Rx switch (Stark Contrasts,
Erlangen, Germany). RF heating was accomplished using the MR RF power amplifier
(8kW peak power, 4ms rect-pulse, U=285V) and TR=40ms resulting in a duty cycle
of 10%. This setup afforded a measured average power of 70W at the antenna. The
heating paradigm consisted of 3×3min RF heating interleaved with 2D MR
thermometry (MRTh) acquisitions. 2D MRTh
was conducted using a proton resonance frequency shift method [6] and dual
gradient-echo technique [7-8] (FOV=(300×300)mm2, TR=61ms, TE1=2.26ms
and TE2=11.44ms, spatial resolution=(1.5×1.5×4)mm3). A fiber optic temperature
sensor (Omniflex, Neoptix, Quebec, Canada) placed 5 mm below the RF antenna was used as
reference.Results
The proposed Tx/Rx switch provided an isolation
of -29dB between Tx port and Rx port during the transmission mode (Table 1). Insertion loss was -0.3dB between
the Tx port and the antenna in transmission mode and -0.3dB between the antenna
and the Rx port in reception mode (Table1). After 3min driving Pavg=85W, Tmax in the circuit was 49.5°C
in the pin diode of the Tx compartment (Fig.3b).
MRI exploiting the proposed high power Tx/Rx
switch and coventional Tx/Rx switches yielded similar image quality (Fig.4a-b). After 9 minutes of RF heating,
the MR thermometry map (Fig.4c) acquired
with the switch showed an increase of ΔT=14.8°C at the position of the fiber optic temperature sensor for
which ΔT=14.1°C was
registered.Discussion and Conclusion
The
proposed high power Tx/Rx switch design provided high isolation and low
insertion loss. By incorporating λ/4 stubs, high transmitter voltages are
blocked effectively from the pin diodes, which afford high power operation. Driving
a Pavg=85W for 3min, the temperature in the circuit of the switch didn’t exceed
50°C, showing low internal losses. Benchmarked against a conventional Tx/Rx switch,
the high power Tx/Rx switch provided similar image quality which demonstrates its
compatibility with the needs of MRI. For the RF heating experiment, the proposed
switch handled an average power of 70W and MRTh, for which the
temperature measurements were well correlated to those from the fiber optic
temperature sensor. In conclusion, the proposed high power Tx/Rx switch is
suitable for MR imaging and RF heating purposes at 297MHz, which bodes very well
for thermal MR applications.Acknowledgements
This
work was funded in part (Y.J., H.W., T.N., L.W.) by the German Federal Ministry
of Education and Research (KMU-innovativ: Medizintechnik, FKZ 13GW0102A, FKZ
13GW0102B).References
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